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Overview Lecture 2 Trapping antiprotons Antihydrogen ATHENA and ATRAP

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Presentation on theme: "Overview Lecture 2 Trapping antiprotons Antihydrogen ATHENA and ATRAP"— Presentation transcript:

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2 Overview Lecture 2 Trapping antiprotons Antihydrogen ATHENA and ATRAP
Making antihydrogen Future developments Applications PET Antiproton therapy? Rocket propulsion??

3 The first nine antihydrogen atoms at CERN (1996)

4 How were the 9 antihydrogen atoms made at LEAR ?
Annihilation of 9 anti-atoms ~ 2 nJ ~ Lifting a mosquito by 1 µm

5 Press reactions (of course)
“Liberation” (France)

6 Two questions to keep you awake
1. With present techniques, what would be the price and delivery time for an 0.5 g anti-hydrogen bomb? The Vatican ? 2. How much antimatter propellant would you need to accelerate a 10-ton spacecraft to 95 % of the speed of light (assuming 100% efficiency)

7 III. TRAPPING ANTIPARTICLES

8 RF trap (“Paul trap”) - / + + / -
A radio-frequency current on the electrodes maintains an alternating electric field that confines charged particles in a small space. + / - - / +

9 Magnetic traps Typical voltages: V For trapping: ~ several kV

10 Special case: Penning trap
Electrodes with hyperbolic shape harmonic forces: Er ~ r, Ez ~ z precise oscillation frequencies !

11 The inertial mass of antiprotons (PS 196, LEAR)
Moving antiprotons induce currents in trap wall The ‘sound of antiprotons’ - at 89.3 MHz (cyclotron frequency) Compare frequency of antiproton and negative hydrogen ions G. Gabrielse Agreement to a precision of 9 x 10-11

12 Reminder: Antiproton Production
Extraction from AD to experiments: 5.3 MeV (~ 0.1 c), 3·107

13 Trapping antiprotons

14 Trap for antiproton capture and storage

15 IV. ANTIHYDROGEN

16 The race for cold antihydrogen
ATHENA and ATRAP - Experiments (Start 2000) Find a way to make cold antihydrogen (done) Trap and cool antihydrogen Precision measurements ATRAP ATHENA

17 Antihydrogen = Hydrogen ??
2S level is metastable (T ~ 120 ms) Two photon laser-spectroscopy (1S-2S energy difference) very narrow line width = high precision: Δν/ν ~ 10-15 Long observation time - need trapped (anti)atoms

18 Antihydrogen milestones
p- and e+ in mixing trap (cooling) Antihydrogen formation AD p- Production (GeV) Deceleration (MeV) Na-22 e+ Production (MeV) Moderation Accumulation (eV) 108 e+ 104 p- Detection of annihilation Trapping (keV) Cooling (meV)

19 Overview - ATHENA / AD-1

20 ATHENA Experiment

21 Positron Accumulation using Buffer Gas
100 million positrons accumulated in 2 min

22 Recombination *D.S. Hall, G. Gabrielse, Phys. Rev. Lett. 77, 1962 (1996)

23 Antihydrogen Detection
Charged particles 2 layers of Si microstrip detectors 511 keV gammas 192 CsI crystals Inner radius 4 cm, thickness ~ 3 cm 70% solid angle coverage Operates at 3 Tesla, 140 Kelvin (C. Regenfus et al., NIM A501, 65 (2003)) Event analysis: Reconstruct vertex from tracks of charged particles Identify pairs of 511 keV γ-rays in time coincidence Measure opening angle between the two γ -rays

24 Antihydrogen - The Movie

25 Antihydrogen Detector

26 First observation of cold antihydrogen
Opening Angle Distribution Peak from back-to-back 511 keV photon pairs Test: peak disappears when positrons are ‘heated’ (RF) Correcting for detection efficiency: > 100,000 anti-atoms

27 Rate of antihydrogen production quite high
Initially > 100 Hz

28 Meanwhile: AD-2 (ATRAP)
Different recombination and detection scheme

29 ATRAP - Recombination scheme
1 2 3 4 5 6 1 Cs atoms are excited to n~50 2 Cs* atoms collide with positron cloud 3 Formation of excited positronium 4 Ps* collides with cold antiprotons 5 Antihydrogen formation (n ~ 45) 6 Antihydrogen detection by ionisation Advantage: Positron attached to ‘resting’ (=cold) antiproton Disadvantage: Low rate (14 antihydrogen atoms detected)

30 ATRAP: Antihydrogen detection by ionisation
Only works for antihydrogen in high-n states (n>35) moving along magnetic axis Field ionization - ‘rip’ positron off, antiproton left and detected by annihilation

31 Present state of the art
Number of produced antihydrogen atoms Energy 1996: 9 (PS210, CERN) 2 GeV 1998: 60 (Fermilab) 3 GeV 2002: > 1,000,000 (AD) eV Antihydrogen production works What about trapping?

32 Next step: Trapping antihydrogen
FUTURE DEVELOPMENTS Next step: Trapping antihydrogen

33 How to trap antihydrogen
How to trap (neutral) antihydrogen? 1) magnetic moment (~ μe+) - ATRAP/ALPHA approach 2) induced electric dipole moment (Stark deceleration) ? 3) Formation of positive antihydrogen ions (additional e+) ??

34 Example: Sextupole magnet
Magnetic bottles ? Example: Sextupole magnet Low field seeking atoms (50%) at r=0 BUT: Very shallow potential (~ 0.07 meV/T) Realistic ΔB ~ T ➪ E < 0.02 meV (reminder: produced antihydrogen has Ekin ~ meV) Trap antihydrogen from low energy ‘Boltzmann tail’ ?

35 Antihydrogen trapping: Laser cooling ?
121 nm laser needed Prototype at MPI Munich … only 50 nW

36 V. APPLICATIONS

37 Applications of antimatter - PET
Insert e+ emitting isotopes (C-11, N-13, O-15, F- 18) into physiologically relevant molecules (O2, glucose, enzymes) and inject into patient. Reconstruct place of positron annihilation with crystal calorimeter

38 Tumour therapy Goal: destroy tumour without (too much) harm to healthy tissue Gammas: exponential decay (peaks at beginning) Charged particles: Bragg peak (Plateau/Peak better for high Z) Antiprotons: like protons, but enhanced Bragg peak from annihilation

39 Antiproton Cell Experiment
Biological effectiveness of antiproton annihilation in cells Additional damage by nuclear fragments of short range Chinese Hamster Cells

40 Antiproton Cell Experiment
Protons Antiprotons Cell survival probability Equal cell mortality for tumour cells with 1/3 radiation dose (= damage to healthy cells) Interesting result - now compare with Carbon ion therapy - dedicated facility ???

41 E = mc2 Antiproton bombs ? 20 kt TNT ~ 8 · 1013 J
0.5 g antimatter g matter 0.5 g antimatter = 0.5·10-3 · 9 · 1016 J = 4.5 · 1013 J Total energy needed (efficiency =10-9 ) : 4.5 · 1022 J EDF discount price CERN (1 kWh = 3.6 · 106 J = 0.1 € ): Price ~ 1015 € Maximum production at CERN ~ 1014 antiprotons / ( year ~ 3 · 107 sec Delivery time ~ 3 billion years

42 Antimatter driven space engines?
10-ton spacecraft at 0.95 c: E = γmc2 ~ 10 · 104 kg = 50 tons of antimatter + 50 t of matter Until somebody finds a clever way around these problems, this will stay fiction: noch nicht ! The End.


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